|Publication number||US5508617 A|
|Application number||US 08/213,678|
|Publication date||Apr 16, 1996|
|Filing date||Mar 16, 1994|
|Priority date||Mar 19, 1993|
|Publication number||08213678, 213678, US 5508617 A, US 5508617A, US-A-5508617, US5508617 A, US5508617A|
|Original Assignee||Hewlett-Packard Company|
|Export Citation||BiBTeX, EndNote, RefMan|
|Patent Citations (4), Non-Patent Citations (2), Referenced by (11), Classifications (9), Legal Events (7)|
|External Links: USPTO, USPTO Assignment, Espacenet|
1. Field of the Invention
The present invention generally relates to an electric power measuring apparatus and an electric power measuring method. More specifically, the present invention is related to an apparatus for and a method of measuring AC power representing a distorted waveform by obtaining a magnitude and a phase of an each frequency component for a voltage and a current, which constitute the distorted AC power.
2. Background of the Invention
Various conventional AC power measuring methods have been proposed. FIG. 1 shows a block diagram for a conventional AC power measuring method which is usually utilized to measure AC power having the frequencies up to several MHz. A voltage v(t) is applied to a voltage input terminal 1, and a current i(t) is supplied to a current input terminal 2. These voltage and current are respectively converted into proper voltage signals through a voltage amplifier 3 and a current-to-voltage converter 4. In response to a sampling pulse derived from a sampling pulse generator 23, instantaneous values of the voltage and the current are sampled by analog-to-digital converters 21 and 22 so as to convert them into digitized data. Then, a calculation is carried out by a computer 9 in accordance with an approximate expression in Formula (2) based generator 23, instantaneous values of the voltage and the current are sampled by analog-to-digital converters 21 and 22 so as to convert them into digitized data. Then, a calculation is carried out by a computer 9 in accordance with an approximate expression in Formula (2) based upon Formula (1) for defining power. It should be noted that symbol "T" denotes a period of fundamental voltage wave and fundamental current wave, and symbol "N" represents the sampling number within one period. If the sampling number N becomes large, then better approximation is achieved. ##EQU1##
In the method shown in FIG. 1, since the frequency characteristics of the voltage amplifier 3 and the current-to-voltage converter 4 are not flat, a large measurement error may occur in the high frequency region. Although the method for correcting the frequency characteristic of the amplitude has been proposed in this field, a phase correction is technically difficult so that a sufficient phase correction cannot be realized. When the frequency of the measurement signal is increased, the operation frequencies of the analog-to-digital converters 21 and 22 must be set to higher values. However, it is difficult to manufacture or purchase such an analog-to-digital converter with high performance in the high frequency range. Furthermore, commercially available high-frequency/high-precision analog-to-digital converters are expensive.
An object of the present invention is to realize an easy method for correcting frequency characteristics of a voltage amplifier and a current-to-voltage converter. Another object is to measure AC power with high precision in a high frequency range with a low-frequency analog-to-digital converter.
In the conventional measuring method, AC power is calculated based upon waveform data of a voltage and a current in a time domain. In the current measuring method, AC power is obtained from magnitudes of the respective frequency components and phases of a voltage and a current in a frequency domain. As represented in Formula (3), AC power with distorted waveforms is equal to the sum of power of the respective frequency components. Therefore, effective values of a voltage and a current are measured for every frequency component, and phase differences between the voltage and the current are measured for every frequency component so that power for each frequency component is calculated. The sum of power calculated for the frequency components becomes desirable AC power. According to this measuring method, an easy frequency-characteristic correction is achieved, and AC power is measured with high precision even in a high frequency range. ##EQU2##
Vn: Effective value of voltage of fundamental wave or n-th harmonic
In: Effective value of current of fundamental wave or n-th harmonic
θn: Phase difference between voltage and current of fundamental wave or n-th harmonic
Pn: Electrical power of fundamental wave or n-th harmonic
The above-described Formula (3) may be derived as follows. Assuming now that no DC component is contained, formula about instantaneous values of a voltage and also a current of a distorted waveform are rexpressed by way of Fourier series: ##EQU3##
It should be noted that symbol "Vmn" denotes a magnitude of voltage, while symbol "Imn" represents a magnitude of current. Symbol "θvn" shows a phase angle of the voltage, and symbol "θin" is a phase angle of the current. Here, assuming that j≠k, power for instantaneous values of this current and voltage is: ##EQU4##
The power is an average value of formula (5) over 1 time period, as shown in formula (1). An average value of an n-th term over 1 time period within a series of a first term in a right hand of Formula (5) is expressed by: ##EQU5##
An average value of a jk-th term over 1 time period within a series of a second term in a right hand of Formula (5) is expressed by: ##EQU6##
As a consequence, an average value of Formula (5) over 1 time period becomes series in which Formula (6) is an n-th term so that formula (3) can be obtained.
FIG. 1 is a block diagram for illustrating one example of the conventional power measuring apparatus.
FIG. 2 is a block diagram of a preferred embodiment according to the present invention.
FIG. 3 is a block diagram for illustrating a method for correcting a voltage measurement error in a power measuring apparatus of the present invention.
FIG. 4 is a block diagram for illustrating a method for correcting a current measurement error in a power measuring apparatus of the present invention.
FIG. 5 illustrates an error model for a measuring device.
FIG. 2 is a block diagram of a preferred embodiment of the present invention. Similar to the above-described prior art, an input voltage v(t) and an input current i(t) are respectively converted into a proper voltage signal by a voltage amplifier 3 and a current-to-voltage converter 4. For measurements, the voltage signals are respectively supplied to mixers 5 and 6. The input signals of the respective mixers are separated to frequency components and converted into intermediate frequencies by sweeping a local signal oscillator 10. These intermediate frequencies are outputted from the mixers 5 and 6. An effective value and a phase of each intermediate frequency signal are respectively measured by vector voltmeters 7 and 8. The measurement results are inputted into a computer 9. In the computer 9, these measurement values are processed in accordance with the above formula (3) to obtain a desirable power value.
As apparent from the conduction process of formula (3), the magnitudes of the voltage and the current which are employed in the power calculation for every frequency component are not limited to effective values, but maximum values or average values thereof may be utilized after being properly converted. As a consequence, average values, crest values, or other measurement values other than effective values may be measured by a vector voltmeter. Also, it is possible to replace these vector voltmeters 7 and 8 by a single vector voltmeter capable of performing a time divisional measurement.
It should be noted that although an infinite number of frequencies is summed in Formula (3), practically speaking, this calculation must be performed with a certain finite number of frequencies. There is no practical problem when the power measurement is stopped at a finite frequency, since the actual signals having the frequencies higher than the finite frequencies are negligible.
In accordance with the present invention, since the power calculation is carried out based on the frequency components in the frequency domain, instead of the waveforms in the time domain, a correction of frequency characteristics is more easily performed than the conventional measuring method. First, an example of an effective value correction of a voltage is represented in FIG. 3. A calibrated voltmeter 12 and a signal source 11 are connected to a voltage input terminal 1. A correction coefficient Kv=|Vs|/|Vms| is obtained from this input voltage |Vs| and the measurement value |Vms| of this measuring device. This calculation of correction coefficient is carried out at preselected frequencies to obtain the correction coefficients "Kv" which will then be stored in a memory unit typically employed in the computer 9. A corrected effective value |Vx| of the voltage may be obtained by the following Formula (8):
It should be noted that symbol |Vm| indicates a measured value of a voltage when power is actually measured. Then, a method of correcting the effective value of the current and the phase difference value between the voltage and the current is realized by applying the conventional OPEN/SHORT/LOAD compensation method of a LCR meter to an arrangement of FIG. 4. An impedance 13 having a known value Zstd (for instance, reference capacitor) is connected to the voltage input terminal 1 and the current input terminal 2, and a sweep signal generator 11 is connected to the voltage terminal 1. With this arrangement, a ratio of the vector measurement value for the voltage to the vector measurement value for the current becomes a measured impedance value. This measured impedance value is expressed as "Zms." Instead of the reference impedance, a measurement value is Zs when a short-circuit plate is connected. Another measurement value is admittance Yo when the input terminals are opened. These measurement values are stored for every frequency. Actually, when power is measured, an impedance Zx corrected by the below-mentioned Formula (9) is calculated based on the impedances Zm obtained from the measurement values of the voltage and the current. The substitution of this Formula (9) will be discussed later. ##EQU7##
With the above conditions, both an effective value |Ix| of the current and a phase difference θx between the voltage and the current are obtained from the following Formulae (10) and (11): ##EQU8##
A correction is made to the frequency of the fundamental wave and the frequencies of the harmonic waves, whereby the frequency characteristics of the measurement system is corrected. It should also be noted that symbols Vn, In, θn respectively correspond to |Vx|, |Ix|, θx at each frequency. Based on these values, the finally corrected power is obtained.
Since the above-described correcting method cannot be employed in the conventional power measuring method, the frequency characteristic of the voltage amplifier must be made flat as much as possible. This results in difficulties of adjustments. This adjustment is one of major causes for the measurement error.
Furthermore, since the signal under measurement is down-converted into the intermediate frequency signal by the frequency conversion in accordance with the present invention, the analog-to-digital (A/D) converter employed in the vector voltmeter may be operated at a relatively low speed. Such a low-speed A/D converter provides sufficient resolution and high precision at low cost. As a result, power can be measured with high precision in comparison to the conventional power measuring method in which the voltage/current waveforms are directly A/D-converted.
The above-explained Formula (9) may be derived as follows. As shown in FIG. 5, an impedance measuring device may be represented by such a model which comprises an ideal measuring device 31 having no error and a two-terminal pair circuit 34 indicative of an error of an actual measuring device at input terminals of the ideal measuring device 31. The left side (the measuring device side) of the terminals 35 and 36 is the actual measuring device whose measurement value is that of the ideal measuring device 31. This corresponds to an impedance as viewed from the right side (an element side to be measured) of the terminals 32 and 33. Assuming now that an impedance of the element to be measured 37 is Zx, a measured value thereof is Zm, and a 4-terminal constant of the 2-terminal pair circuit 34 is ABCD. This measurement value Zm is given as follows: ##EQU9##
Here, assumed k1 =B/A, k2 =C/A, and k3 =D/A. This formula may be converted as follows: ##EQU10##
If the three unknown numbers k1, k2, k3 become known, a true value Zx whose error has been corrected can be obtained from Formula (14). To this end, measurements are made of the three different known impedances. The known value is substituted for the true value Zx of Formula (15), and the measurement values are substituted for Zm. Thus, simultaneous equations are established. From the simultaneous equations, k1, k2 and k3 indicated in the Formula (16) are obtained. In this case, the three known impedances are respectively selected as an open impedance, a short-circuit impedance, and a reference impedance. Their measurement values are respectively 1/Zo=Yo, Zs, Zms, and the reference impedance is Zstd. ##EQU11##
These values are substituted for formula (14) to obtain formula (9).
The correction for the frequency characteristics of the measurement system is readily performed in accordance with the present invention. Since the measurement is obtained with a relatively low-speed A/D converter, sufficient resolution and high precision are achieved. The power is measured with high precision even in a high frequency range although such a power measurement in the high frequency range cannot be executed by the conventional measuring method.
It should be noted that the circuit arrangements and the devices employed in the above-explained preferred embodiments are not limited thereto, but may be modified without departing from the technical scope of the present invention.
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|U.S. Classification||324/379, 324/107, 324/141|
|International Classification||G01R21/133, G01R35/00, G01R21/06|
|Cooperative Classification||G01R21/06, G01R21/133|
|Jun 17, 1994||AS||Assignment|
Owner name: HEWLETT-PACKARD COMPANY, CALIFORNIA
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Effective date: 19940401
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|Apr 28, 2000||AS||Assignment|
Owner name: HEWLETT-PACKARD COMPANY, A DELAWARE CORPORATION, C
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|May 30, 2000||AS||Assignment|
Owner name: AGILENT TECHNOLOGIES INC, CALIFORNIA
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